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3.3.5 Radiative stars

• Repeat for mass continuity, energy generation and radiative energy transport to get 4 simultaneous eqs in the four indices α...

• Determinant of matrix in LHS is:

Denotes diffusive radiative transfer

in energy transport equation; Drad ≠ 0. AS 4013 Stellar Physics

3.3.6 Solutions

• Solutions of matrix equation are:

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Page ‹#› 3.3.7 Convective stars

• Energy transport by fully adiabatic convection gives:

• Matrix equation becomes:

• Slightly simpler determinant and solutions.

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3.3.8 Upper-main sequence stars • Dominant opacity source is electron scattering which is independent of ρ, T so n = s = 0. • Energy source is thermonuclear CNO cycle for which λ = 1 and ν ~ 15.

: (P ∝ ρT) so χρ=χΤ=1. • Substitute these values in equations for radiative stars to get:

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Page ‹#› Upper MS stars

• Hence for M > 1 MSun:

• Not too bad: recall that L ∝ M3.6 for high-mass stars in binaries. • Average density falls, rises with increasing mass. • But we’ve made some major approximations and haven’t solved any DEs!

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Interlude: The Virial Theorem

• Whole system is in equilibrium if hydrostatic equilibrium is satisfied at all r. • Hence get relation between average internal and gravitational PE of whole system.

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Page ‹#› Average internal pressure

Volume-averaged Gravitational PE pressure of system of system

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Pressure: nonrelativistic gas

Fundamentally important result! Means that tightly bound systems in hydrostatic equilibrium have high particle KE, i.e. they’re HOT.

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Page ‹#› Pressure: ultra-relativistic gas

• For a gas of ultra-relativistic particles:

• As UR limit is approached, binding energy decreases and system is easily disrupted.

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Common ultra-relativistic gases

• Radiation-pressure dominated: • Pressure from photons, UR by definition! – e.g. supermassive stars.

• Degenerate electron-pressure dominated: • If electron temperature becomes very high – e.g. massive white dwarfs.

• Both to be discussed in more detail later.

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